# Terminal velocity of two equally shaped/sized objects with different masses?

I've tried doing research on this and there are some similar questions. However, they have slightly different scenarios and to make sure I understand things perfectly, I wanted to word it into my own words and confirm that my thought process is correct. I am just getting back into physics after a decade of not doing anything remotely related, so I'd like to make sure I'm not confusing things.

We have two objects that are the exact same size and shape. Let's call them A and B.
A is twice the mass of B.

Both are dropped from an airplane at the same time.

Am I correct to say that since B is half the mass of A, it will reach its terminal velocity much sooner, producing 0 acceleration from there on.

A, on the other hand, will continue accelerating until the positive force from the air resistance equals its weight, at which point it reaches its terminal velocity and 0 acceleration.

A will have a higher terminal velocity and reach the ground sooner than B, because A was accelerating for a longer period of time.

EDIT: Changed from mass to weight, due to the fact that weight is the force pushing those two objects towards the Earth.

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The edit was not really necessary - when applied to 2 objects in the same reference frame, mass and weight are pretty much interchangeable. – Pranav Hosangadi Sep 2 '13 at 3:29
Also, I don't really see your question. If you meant to ask if your reasoning is correct, then my answer would be that it is. This is why a person with a parachute reaches the ground much later than a person without one. – Pranav Hosangadi Sep 2 '13 at 3:37
@PranavHosangadi Yes, that's actually exactly what I asked. In the first paragraph I'm asking to confirm that my reasoning is correct. I ask, "Am I correct to..." – B.K. Sep 2 '13 at 3:40

Yes, although I don't think it's totally obvious that your statements are true. Let's assume that the drag force on a given object is \begin{align} \mathbf F_\mathrm{drag} = -\frac{1}{2}\rho AC_dv\mathbf v \end{align} where $\rho$ is the mass density of the fluid in which it moves, $A$ is its cross-sectional area, $C_d$ is its drag coefficient, $\mathbf v$ is its velocity, and $v=|\mathbf v|$ is its speed. Then Newton's Second Law gives the following equation of motion for an object falling near the surface of the Earth under the influence of gravity: \begin{align} ma = m g -\frac{1}{2}\rho AC_d v^2 \end{align} So that the acceleration of the object is \begin{align} a = g - \frac{1}{2}\frac{\rho AC_d}{m}v^2 \end{align} In particular, for a fixed cross-sectional area, increasing the mass of the object will increase its acceleration because the second term will be smaller in magnitude. But that also means that the object's speed with increase faster, so that the second term will grow faster; there are competing affects. So which one wins out? Well, the equation of motion can be looked upon as a differential equation for the velocity $v(t)$ as a function of time; \begin{align} \dot v(t) = g-\frac{1}{2}\frac{\rho AC_d}{m} v(t)^2 \end{align} With the initial condition $v(0) = 0$, namely if you just drop the object, the solution (thanks to to Stephen Wolfram) is \begin{align} v(t) = \sqrt{\frac{2gm}{AC_d\rho}}\tanh\left(\sqrt\frac{AC_dg\rho}{2m}t\right) \end{align} Let's plot this function for some different mass values but keeping all other parameters the same